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Related papers: IsoDAR@KamLAND: A Conceptual Design Report for the…

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This document describes requirements for the caverns to house the cyclotron, beam transport line, and target systems; issues associated with transport and assembly of components on the site; electrical power, cooling and ventilation; as…

Instrumentation and Detectors · Physics 2019-08-14 Jose R. Alonso , K. Nakamura

This whitepaper reviews design options for the IsoDAR electron antineutrino source. IsoDAR is designed to produce $2.6 \times 10^{22}$ electron antineutrinos per year with an average energy of 6.4 MeV, using isotope decay-at-rest. Aspects…

This Conceptual Design Report addresses the site-specific issues associated with the deployment of the IsoDAR experiment at the Yemilab site. IsoDAR@Yemilab pairs the IsoDAR cyclotron-driven $\bar{\nu}_e$ source with the proposed Liquid…

IsoDAR seeks to place a high-power-cyclotron and target combination, as an intense source of $\bar{\nu}_e$ at the level of $\sim 10^{23}$/year, close to a kiloton-scale neutrino detector in order to gain sensitivity to very short-baseline…

High Energy Physics - Experiment · Physics 2022-04-06 J. Alonso , C. A. Argüelles , A. Bungau , J. M. Conrad , B. Dutta , Y. D. Kim , E. Marzec , D. Mishins , S. H. Seo , M. Shaevitz , J. Spitz , A. Thompson , L. Waites , D. Winklehner

IsoDAR@Yemilab is a novel isotope-decay-at-rest experiment that has preliminary approval to run at the Yemi underground laboratory (Yemilab) in Jeongseon-gun, South Korea. In this technical report, we describe in detail the considerations…

This Preliminary Design Report (PDR) describes the IsoDAR electron-antineutrino source in two volumes which are mostly site-independent and describe the cyclotron driver providing a 60 MeV, 10 mA proton beam (Volume I); and the medium…

Configurations of the IsoDAR and DAE{\delta}ALUS decay-at-rest neutrino experiments are described. Injector and cyclotron developments aimed at substantial increases in beam current are discussed. The IsoDAR layout and target are described,…

Instrumentation and Detectors · Physics 2016-11-14 Jose R. Alonso

The primary goal of KamLAND is a search for the oscillation of $\bar{\nu}_{\rm e}$$'$s emitted from distant power reactors. The long baseline, typically 180 km, enables KamLAND to address the oscillation solution of the solar neutrino…

High Energy Physics - Experiment · Physics 2015-06-22 Atsuto Suzuki

The IsoDAR antineutrino source, which produces a flux from 8Li isotope decay at rest, when paired with the proposed JUNO (Jiangmen Underground Neutrino Observatory) detector, has unprecedented sensitivity to anti-nu_e disappearance for…

High Energy Physics - Experiment · Physics 2014-03-19 J. M. Conrad , M. H. Shaevitz

This Preliminary Design Report (PDR) describes the IsoDAR electron-antineutrino source in two volumes which are mostly site-independent and describe the cyclotron driver providing a 60 MeV, 10 mA proton beam (this Volume); and the medium…

KamLAND is a reactor neutrino oscillation experiment with a very long baseline. This experiment successfully measured oscillation phenomena of reactor antineutrinos coming mainly from 53 reactors in Japan. In order to extract the results,…

Data Analysis, Statistics and Probability · Physics 2008-11-26 K. Nakajima , K. Inoue , K. Owada , F. Suekane , A. Suzuki , G. Hirano , S. Kosaka , T. Ohta , H. Tanaka

IsoDAR provides a pure and intense $\bar \nu_e$ source with an average energy of 6.5 MeV produced through $^8$Li $\beta$-decay. This source can be paired with a large scintillator detector, such as KamLAND, to produce a sample of $\bar…

High Energy Physics - Experiment · Physics 2014-04-23 J. M. Conrad , M. H. Shaevitz , I. Shimizu , J. Spitz , M. Toups , L. Winslow

We present results of a study of neutrino oscillation based on a 766 ton-year exposure of KamLAND to reactor anti-neutrinos. We observe 258 \nuebar\ candidate events with energies above 3.4 MeV compared to 365.2 events expected in the…

High Energy Physics - Experiment · Physics 2012-08-27 The KamLAND Collaboration

The Kamioka Liquid scintillator Anti-Neutrino Detector (KamLAND) is sensitive to the neutrino event spectrum from (mainly Japanese) nuclear reactors in both the energy domain and the time domain. While the energy spectrum of KamLAND events…

High Energy Physics - Phenomenology · Physics 2009-10-07 G. L. Fogli , E. Lisi , A. Palazzo , A. M. Rotunno

We have successfully built and operated a source deployment system for the KamLAND detector. This system was used to position radioactive sources throughout the delicate 1-kton liquid scintillator volume, while meeting stringent material…

Instrumentation and Detectors · Physics 2012-08-27 The KamLAND Collaboration

We give an alternative description of the new data produced in the KamLAND experiment, assuming the existence of a natural nuclear reactor on the boundary of the liquid and solid phases of the Earth's core. Analyzing the uncertainty of…

The Kamioka Liquid scintillator Anti-Neutrino Detector (KamLAND) is collecting antineutrino events generated by nuclear reactors and by Thorium and Uranium decay in the Earth interior. We comment on a systematic approach to the evaluation…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. L. Fogli , E. Lisi , A. Palazzo , A. M. Rotunno

The International Design Study for the Neutrino Factory (the IDS-NF) was established by the community at the ninth "International Workshop on Neutrino Factories, super-beams, and beta- beams" which was held in Okayama in August 2007. The…

High Energy Physics - Experiment · Physics 2025-08-01 R. J. Abrams , S. K. Agarwalla , A. Alekou , C. Andreopoulos , C. M. Ankenbrandt , S. Antusch , M. Apollonio , M. Aslaninejad , J. Back , P. Ballett , G. Barker , K. B. Beard , E. Benedetto , J. R. J. Bennett , J. S. Berg , S. Bhattacharya , V. Blackmore , M. Blennow , A. Blondel , A. Bogacz , M. Bonesini , C. Bontoiu , C. Booth , C. Bromberg , S. J. Brooks , A. Bross , O. Caretta , A. Cervera-Villanueva , S. Choubey , D. Cline , J. Cobb , P. Coloma , L. Coney , M. A. C. Cummings , T. Davenne , A. de Gouvea , C. Densham , X. Ding , A. Donini , P. Dornan , M. Dracos , F. Dufour , R. Eccleston , R. Edgecock , I. Efthymiopoulos , M. Ellis , E. Fernandez-Martinez , R. Fernow , G. Flanagan , J. C. Gallardo , R. Gandhi , R. Garoby , B. Gavela , S. Geer , S. Gilardoni , J. J. Gomez-Cadenas , S. Goswami , V. B. Graves , R. Gupta , G. Hanson , P. Harrison , T. Hart , P. Hernandez , P. Huber , D. Indumathi , R. P. Johnson , C. Johnstone , Y. Karadzhov , D. Kelliher , H. Kirk , J. Kopp , Y. Kudenko , Y. Kuno , A. Kurup , P. Kyberd , A. Laing , T. Li , M. Lindner , K. Long , J. Lopez Pavon , P. Loveridge , S. Machida , D. Majumdar , M. Maltoni , J. Martin-Albo , M. Martini , R. Matev , K. T. McDonald , A. McFarland , D. Meloni , M. Mezzetto , P. Migliozzi , S. R. Mishra , N. Mokhov , N. Mondal , J. Morfin , Y. Mori , V. Morozov , D. Neuffer , T. Ota , V. Palladino , S. Parke , S. Pascoli , J. Pasternak , J. Peltoniemi , R. Petti , T. Planche , M. Popovic , J. Pozimski , G. Prior , C. Prior , G. Rees , S. Rigolin , T. J. Roberts , Y. Roblin , C. Rogers , R. Samulyak , T. Schwetz , N. Simos , N. Sinha , G. Skoro , P. Snopok , F. J. P. Soler , N. Souchlas , J. Strait , D. Stratakis , S. Striganov , J. Tang , J. W. G. Thomason , L. Tortora , R. Tsenov , W. Winter , H. Witte , O. Yasuda , C. Y. Yoshikawa , M. Zisman
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